Check force on energy

It is common practise to use the potential energy as a collective energy. Some MD codes thus pass the potential energy to PLUMED and PLUMED can then apply forces on this collective variable. We test that any forces that PLUMED applies on the potential energy are correctly passed back to the MD code by doing the following test. We first run a short simulation at $T$ K with a timestep of $\tau$ ps. During the course of this simulation we monitor the potential energy using the following PLUMED input:

Click on the labels of the actions for more information on what each action computes
tested on2.10
tested onmaster
e: ENERGYCalculate the total potential energy of the simulation box. More details
v: VOLUMECalculate the volume the simulation box. More details
PRINTPrint quantities to a file. More details ARGthe labels of the values that you would like to print to the file=e,v FILEthe name of the file on which to output these quantities=energy1

We then run a second simulation (starting from identical conditions) at a temperature of $T\alpha$ and with a timestep of $\tau/\sqrt(\alpha)$. The thermostat and barostat relaxation times are similarly divided by $\sqrt(\alpha)$. In the tests that are run on this website we set $\sqrt(\alpha)=1.1$. The PLUMED file above is used when this test is run but a different time series of energy values is recorded as the MD parameters in this second simulation are different.

If PLUMED is working correctly we should be able to recapture the time series of energy values for the first simulation by running an MD simulation with the modified parameters that were used in the second simulation and the following PLUMED input file:

Click on the labels of the actions for more information on what each action computes
tested on2.10
tested onmaster
e: ENERGYCalculate the total potential energy of the simulation box. More details
v: VOLUMECalculate the volume the simulation box. More details
# slope is such that 
PRINTPrint quantities to a file. More details ARGthe labels of the values that you would like to print to the file=e FILEthe name of the file on which to output these quantities=energy2
# slope should be (alpha-1)=0.21
RESTRAINTAdds harmonic and/or linear restraints on one or more variables. More details ATthe position of the restraint=0.0 ARGthe values the harmonic restraint acts upon=e SLOPE specifies that the restraint is linear and what the values of the force constants on each of the variables are=0.21

In other words, when forces are passed correctly the time series for the energies and volumes from the first and third of these calculations should be identical.

To determine if PLUMED passes this test we calculate the difference between the time series that were observed in the first and third simulations described above. We then divide this by the difference between the first and second time series.

An NPT version of this calculation is performed as well as an NVT calculation if the virial is passed to PLUMED.

Trajectories

  1. Input and output files for the unpeturbed calculation are available in this zip archive

  2. Input and output files for the peturbed calculation are available in this zip archive

  3. Input and output files for the peturbed calculation in which a PLUMED restraint is used to undo the effect of the changed MD parameters are available in this zip archive

Results

Original With PLUMED Effect of peturbation % Difference
-18174.8223 11.6346 -18174.8223 11.6346 0.0000 0.0000 0.0000 0.0000
-18171.8203 11.6346 -18193.2891 11.6346 6.8730 0.0000 312.3615 0.0000
-18194.2520 11.6475 -18235.0137 11.6321 22.5078 0.0054 181.1003 284.9140
-18166.7832 11.6475 -18290.7832 11.6321 18.6758 0.0054 663.9615 284.9140
-18153.8594 11.6475 -18334.3066 11.6321 21.6855 0.0054 832.1084 284.9140
-18136.0703 11.6475 -18361.1836 11.6321 23.0332 0.0054 977.3425 284.9140
-18119.0371 11.6475 -18370.7949 11.6321 24.6934 0.0054 1019.5365 284.9140
-18108.6797 11.6475 -18368.9199 11.6321 28.2246 0.0054 922.0331 284.9140
-18108.1133 11.6475 -18363.5371 11.6321 33.5273 0.0054 761.8374 284.9140
-18116.1602 11.6475 -18360.5996 11.6321 38.7422 0.0054 630.9387 284.9140
-18127.9922 11.6475 -18361.9727 11.6321 41.2305 0.0054 567.4941 284.9140
-18138.1406 11.6475 -18366.4883 11.6321 39.7539 0.0054 574.4031 284.9140
-18144.2012 11.6475 -18372.7656 11.6321 36.1875 0.0054 631.6116 284.9140
-18148.9043 11.6475 -18381.7129 11.6321 35.1836 0.0054 661.6965 284.9140
-18158.1758 11.6475 -18395.9648 11.6321 40.9414 0.0054 580.8034 284.9140
-18175.8145 11.6475 -18416.2930 11.6321 52.7617 0.0054 455.7822 284.9140
-18198.8613 11.6475 -18438.5371 11.6321 63.4805 0.0054 377.5583 284.9140
-18218.5547 11.6475 -18454.5137 11.6321 63.9922 0.0054 368.7309 284.9140
-18225.8359 11.6475 -18457.1250 11.6321 50.0137 0.0054 462.4517 284.9140
-18217.2734 11.6475 -18445.2832 11.6321 25.6836 0.0054 887.7642 284.9140

The table below includes some of the results from the calculation. The columns contain:

  1. Time series for the energy and volume that were obtained from the simulation at $T$ K, $x_{md}$.
  2. Time series for the energy and volume that were obtained from the simulation at $\alpha T$ K and in which PLUMED applied a restraint on the energy, $x_{pl}$.
  3. The absolute value of the difference between the time series of energies and volumes that were obtained from the simulations running at $T$ K and $\alpha T$ K, $\vert x_{md}’-x_{md} \vert$. No PLUMED restraints were applied in either of these simulations.
  4. The values of $100\frac{\vert x_{md} - x_{pl}\vert }{ \vert x_{md}’-x_{md} \vert}$.

If the PLUMED interface is working correctly the first two sets of numbers should be identical and the final column should be filled with zeros.

Graphical representation (beta)

A visualization of the table above:
engvir_master